Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -997.050427 |
| Energy at 298.15K | -997.055273 |
| Nuclear repulsion energy | 194.889032 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3260 |
2952 |
0.00 |
|
|
|
| 2 |
Ag |
1616 |
1464 |
0.00 |
|
|
|
| 3 |
Ag |
1464 |
1325 |
0.00 |
|
|
|
| 4 |
Ag |
1129 |
1023 |
0.00 |
|
|
|
| 5 |
Ag |
828 |
750 |
0.00 |
|
|
|
| 6 |
Ag |
322 |
292 |
0.00 |
|
|
|
| 7 |
Au |
3342 |
3026 |
4.61 |
|
|
|
| 8 |
Au |
1238 |
1121 |
0.85 |
|
|
|
| 9 |
Au |
829 |
751 |
1.70 |
|
|
|
| 10 |
Au |
126 |
114 |
8.52 |
|
|
|
| 11 |
Bg |
3318 |
3005 |
0.00 |
|
|
|
| 12 |
Bg |
1401 |
1268 |
0.00 |
|
|
|
| 13 |
Bg |
1097 |
993 |
0.00 |
|
|
|
| 14 |
Bu |
3265 |
2957 |
20.70 |
|
|
|
| 15 |
Bu |
1614 |
1462 |
7.16 |
|
|
|
| 16 |
Bu |
1367 |
1237 |
53.10 |
|
|
|
| 17 |
Bu |
775 |
701 |
137.71 |
|
|
|
| 18 |
Bu |
234 |
212 |
10.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13612.3 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12325.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.757 |
0.000 |
| C2 |
0.000 |
-0.757 |
0.000 |
| Cl3 |
-1.691 |
1.348 |
0.000 |
| Cl4 |
1.691 |
-1.348 |
0.000 |
| H5 |
0.478 |
1.152 |
0.882 |
| H6 |
0.478 |
1.152 |
-0.882 |
| H7 |
-0.478 |
-1.152 |
0.882 |
| H8 |
-0.478 |
-1.152 |
-0.882 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5144 | 1.7909 | 2.7003 | 1.0784 | 1.0784 | 2.1569 | 2.1569 |
C2 | 1.5144 | | 2.7003 | 1.7909 | 2.1569 | 2.1569 | 1.0784 | 1.0784 | Cl3 | 1.7909 | 2.7003 | | 4.3249 | 2.3495 | 2.3495 | 2.9156 | 2.9156 | Cl4 | 2.7003 | 1.7909 | 4.3249 | | 2.9156 | 2.9156 | 2.3495 | 2.3495 | H5 | 1.0784 | 2.1569 | 2.3495 | 2.9156 | | 1.7642 | 2.4950 | 3.0557 | H6 | 1.0784 | 2.1569 | 2.3495 | 2.9156 | 1.7642 | | 3.0557 | 2.4950 | H7 | 2.1569 | 1.0784 | 2.9156 | 2.3495 | 2.4950 | 3.0557 | | 1.7642 | H8 | 2.1569 | 1.0784 | 2.9156 | 2.3495 | 3.0557 | 2.4950 | 1.7642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.279 |
|
C1 |
C2 |
H7 |
111.485 |
| C1 |
C2 |
H8 |
111.485 |
|
C2 |
C1 |
Cl3 |
109.279 |
| C2 |
C1 |
H5 |
111.485 |
|
C2 |
C1 |
H6 |
111.485 |
| Cl3 |
C1 |
H5 |
107.323 |
|
Cl3 |
C1 |
H6 |
107.323 |
| Cl4 |
C2 |
H7 |
107.323 |
|
Cl4 |
C2 |
H8 |
107.323 |
| H5 |
C1 |
H6 |
109.770 |
|
H7 |
C2 |
H8 |
109.770 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.218 |
|
|
|
| 2 |
C |
-0.218 |
|
|
|
| 3 |
Cl |
-0.172 |
|
|
|
| 4 |
Cl |
-0.172 |
|
|
|
| 5 |
H |
0.195 |
|
|
|
| 6 |
H |
0.195 |
|
|
|
| 7 |
H |
0.195 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-42.991 |
4.747 |
0.000 |
| y |
4.747 |
-40.389 |
0.000 |
| z |
0.000 |
0.000 |
-37.632 |
|
| Traceless |
| | x | y | z |
| x |
-3.980 |
4.747 |
0.000 |
| y |
4.747 |
-0.078 |
0.000 |
| z |
0.000 |
0.000 |
4.058 |
|
| Polar |
| 3z2-r2 | 8.116 |
| x2-y2 | -2.602 |
| xy | 4.747 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.254 |
-1.751 |
0.000 |
| y |
-1.751 |
6.335 |
0.000 |
| z |
0.000 |
0.000 |
5.038 |
<r2> (average value of r
2) Å
2
| <r2> |
200.401 |
| (<r2>)1/2 |
14.156 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -997.047434 |
| Energy at 298.15K | -997.052420 |
| HF Energy | -997.047434 |
| Nuclear repulsion energy | 202.099843 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3306 |
2993 |
0.97 |
|
|
|
| 2 |
A |
3248 |
2941 |
29.28 |
|
|
|
| 3 |
A |
1601 |
1450 |
0.04 |
|
|
|
| 4 |
A |
1464 |
1326 |
27.42 |
|
|
|
| 5 |
A |
1333 |
1207 |
0.46 |
|
|
|
| 6 |
A |
1125 |
1018 |
0.88 |
|
|
|
| 7 |
A |
1029 |
932 |
15.22 |
|
|
|
| 8 |
A |
710 |
643 |
28.71 |
|
|
|
| 9 |
A |
279 |
253 |
1.06 |
|
|
|
| 10 |
A |
122 |
110 |
1.23 |
|
|
|
| 11 |
B |
3319 |
3005 |
6.14 |
|
|
|
| 12 |
B |
3236 |
2930 |
3.95 |
|
|
|
| 13 |
B |
1596 |
1445 |
8.76 |
|
|
|
| 14 |
B |
1437 |
1302 |
54.89 |
|
|
|
| 15 |
B |
1257 |
1138 |
0.46 |
|
|
|
| 16 |
B |
974 |
882 |
18.09 |
|
|
|
| 17 |
B |
740 |
670 |
39.86 |
|
|
|
| 18 |
B |
439 |
397 |
9.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13606.0 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12320.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.299 |
0.695 |
0.882 |
| C2 |
-0.299 |
-0.695 |
0.882 |
| Cl3 |
-0.299 |
1.703 |
-0.464 |
| Cl4 |
0.299 |
-1.703 |
-0.464 |
| H5 |
0.018 |
1.201 |
1.796 |
| H6 |
1.374 |
0.661 |
0.805 |
| H7 |
-0.018 |
-1.201 |
1.796 |
| H8 |
-1.374 |
-0.661 |
0.805 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5133 | 1.7852 | 2.7505 | 1.0811 | 1.0787 | 2.1282 | 2.1553 |
C2 | 1.5133 | | 2.7505 | 1.7852 | 2.1282 | 2.1553 | 1.0811 | 1.0787 | Cl3 | 1.7852 | 2.7505 | | 3.4586 | 2.3367 | 2.3446 | 3.6905 | 2.8909 | Cl4 | 2.7505 | 1.7852 | 3.4586 | | 3.6905 | 2.8909 | 2.3367 | 2.3446 | H5 | 1.0811 | 2.1282 | 2.3367 | 3.6905 | | 1.7641 | 2.4020 | 2.5274 | H6 | 1.0787 | 2.1553 | 2.3446 | 2.8909 | 1.7641 | | 2.5274 | 3.0503 | H7 | 2.1282 | 1.0811 | 3.6905 | 2.3367 | 2.4020 | 2.5274 | | 1.7641 | H8 | 2.1553 | 1.0787 | 2.8909 | 2.3446 | 2.5274 | 3.0503 | 1.7641 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.731 |
|
C1 |
C2 |
H7 |
109.095 |
| C1 |
C2 |
H8 |
111.409 |
|
C2 |
C1 |
Cl3 |
112.731 |
| C2 |
C1 |
H5 |
109.095 |
|
C2 |
C1 |
H6 |
111.409 |
| Cl3 |
C1 |
H5 |
106.619 |
|
Cl3 |
C1 |
H6 |
107.314 |
| Cl4 |
C2 |
H7 |
106.619 |
|
Cl4 |
C2 |
H8 |
107.314 |
| H5 |
C1 |
H6 |
109.526 |
|
H7 |
C2 |
H8 |
109.526 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.220 |
|
|
|
| 2 |
C |
-0.220 |
|
|
|
| 3 |
Cl |
-0.161 |
|
|
|
| 4 |
Cl |
-0.161 |
|
|
|
| 5 |
H |
0.186 |
|
|
|
| 6 |
H |
0.195 |
|
|
|
| 7 |
H |
0.186 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
3.007 |
3.007 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.509 |
1.363 |
0.000 |
| y |
1.363 |
-42.967 |
0.000 |
| z |
0.000 |
0.000 |
-35.372 |
|
| Traceless |
| | x | y | z |
| x |
1.660 |
1.363 |
0.000 |
| y |
1.363 |
-6.527 |
0.000 |
| z |
0.000 |
0.000 |
4.867 |
|
| Polar |
| 3z2-r2 | 9.733 |
| x2-y2 | 5.458 |
| xy | 1.363 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.310 |
-0.561 |
0.000 |
| y |
-0.561 |
7.201 |
0.000 |
| z |
0.000 |
0.000 |
6.659 |
<r2> (average value of r
2) Å
2
| <r2> |
164.615 |
| (<r2>)1/2 |
12.830 |